Isomorphism and equivariance of the Whittaker-space embedding

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Let O⊂XQ,n\mathcal{O}\subset\mathscr{X}_{Q,n} be a WW-orbit, let I(χ)I(\chi) be the relevant principal-series representation, and let Wh⁡ψ(I(χ))O\operatorname{Wh}_\psi(I(\chi))_\mathcal{O} and Wh⁡ψ(I(χ))O♯\operatorname{Wh}_\psi(I(\chi))_\mathcal{O}^{\sharp} denote the corresponding Whittaker subspaces. Let T(w,χ)T(w,\chi) and T(w,χ)♯T(w,\chi)^{\sharp} be the homomorphisms induced by the intertwining operator T(w,χ)T(w,\chi), and let ι(χ)ψ,O\iota(\chi)_{\psi,\mathcal{O}} be the natural embedding.

Whittaker-space isomorphism conjecture. For every WW-orbit O⊂XQ,n\mathcal{O}\subset\mathscr{X}_{Q,n}, the embedding is an isomorphism

ι(χ)ψ,O:Wh⁡ψ(I(χ))O≃Wh⁡ψ(I(χ))O♯.\iota(\chi)_{\psi,\mathcal{O}}:\operatorname{Wh}_\psi(I(\chi))_\mathcal{O}\simeq\operatorname{Wh}_\psi(I(\chi))_\mathcal{O}^{\sharp}.

Moreover, it is equivariant in the sense that

ι(wχ)ψ,O∘T(w,χ)ψ,O=T(w,χ)ψ,O♯∘ι(χ)ψ,O.\iota({}^w\chi)_{\psi,\mathcal{O}}\circ T(w,\chi)_{\psi,\mathcal{O}}=T(w,\chi)_{\psi,\mathcal{O}}^{\sharp}\circ\iota(\chi)_{\psi,\mathcal{O}}.

This identifies the two descriptions of the relevant Whittaker spaces and makes them compatible with intertwining operators. The supplied text gives no resolution status beyond the assertion itself.

References

Primary source

Fan Gao, Nadya Gurevich and Edmund Karasiewicz, “Genuine pro-p Iwahori–Hecke algebras, Gelfand–Graev representations, and some applications”, arXiv:2204.13053 (2022).

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